The photodissociation of phenol is a prototype of the photoinduced hydrogen detachment reaction. The dissociation rates of phenol through the excited S 1 state are calculated with the quantum instanton method in full dimensionality. The Arrhenius plot of the rates shows that the quantum tunneling dominates the O H bond dissociation at low temperatures. The degrees of freedom of phenyl ring (C 6 H 5 ) play extremely important roles in the dissociation of phenol. Fixing the phenyl ring at the equilibrium geometry can only provide reliable rates between 400 K and 800 K. The motions of phenyl ring have an impact on enhancing the dissociation by lowering the free energy barrier. The larger the amplitudes of the phenyl ring motions are, the more the free energy barrier will be reduced. The dissociation rates of C 6 H 5 OH are much larger than those of C 6 H 5 OD, which is due to the zero-point energy and entropy effects. K E Y W O R D S free energy barrier, kinetic isotope effect, quantum tunneling, rate constant, zero-point energy 1 | INTRODUCTIONThe photodissociation of phenol to produce H and phenoxyl radical is a prototype of photoinduced hydrogen elimination reaction. Because phenol is one of the chromophores in many natural compounds, the investigation of photochemistry of phenol [1][2][3] provides a useful guide to the study of complex biological molecules, such as peptides and DNA bases.A variety of experimental techniques [4][5][6][7] have been developed by the scientists to explore the photodissociation of phenol, such as H Rydberg atom photofragment translational spectroscopy, [8,9] velocity map ion imaging, [10][11][12][13] high-resolution time-of-flight spectra [14] and multimass ion imaging. [15] Ratzer et al. [16] measured the lifetimes of excited states, and observed the increased O H bond, the shortened C O bond and the expanded aromatic ring on electronic excitation. Tseng et al. [15] detected the cleavage of O H bond at 193 nm and 248 nm. Hause et al. [10] showed that the excitation of O H stretching led to the formation of excited state products. Pino et al. [17] clarified the position and substituent effects of phenol. Nix et al. [4] and Ashfold et al. [5,14] reported that the fragmentation of phenol involved nuclear motion on the [1] πσ* potential energy surface.The electronic structure calculations [18][19][20] have revealed that the photodissociation of phenol to produce H and phenoxyl radical involves the three lowest electronic states, 1 ππ, 1 ππ*, and 1 πσ*. The equilibrium structures and the vertical excitation energies of these states have been predicted by several authors at various levels of theory. Lorentzon et al. [21] obtained 27 singlet states in the range of 4.53 eV-7.84 eV by the complete active space perturbation theory to second-order method (CASPT2). Fang [22] characterized the structures of electronic ground and excited states of phenol at the complete active space self-consistent field (CASSCF) level. Sobolewski and Domcke [23] predicted the vertical excitation energies using a...